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arxiv: 2604.12828 · v1 · submitted 2026-04-14 · ❄️ cond-mat.mtrl-sci · cond-mat.str-el

Order-disorder transition and Na-ion redistribution in NASICON-type Na₃FeCr(PO₄)₃

Pith reviewed 2026-05-10 14:38 UTC · model grok-4.3

classification ❄️ cond-mat.mtrl-sci cond-mat.str-el
keywords NASICONorder-disorder transitionNa-ion redistributionstructural transitionsynchrotron X-ray diffractioncalorimetryNa-vacancy orderingpolyanionic framework
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The pith

Na-ion redistribution governs the order-disorder transition in NASICON-type Na3FeCr(PO4)3 while the host framework remains unchanged.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The paper shows that Na3FeCr(PO4)3 undergoes a symmetry-lowering transition on heating from a monoclinic phase that has long-range ordered Na vacancies to a rhombohedral phase with statistically disordered Na ions. The transition occurs through movement of Na ions out of one set of sites and into another set inside the conduction channels. The iron-chromium-phosphate framework stays fixed in position and bonding throughout. A reader would care because this identifies the Na sublattice as the active element that sets the material's symmetry, volume, and phase stability, which directly affects how well such compounds can conduct ions in batteries or solid electrolytes.

Core claim

The [FeCr(PO4)3] polyanionic framework remains essentially unchanged across the transition from the monoclinic C2/c phase with long-range Na-vacancy order to the rhombohedral R-3c phase with statistical Na disorder. The transition is instead driven by progressive depopulation of Na(1) sites and transfer to the Na(2) sublattice, producing a discontinuous expansion along the c-axis and an increase in unit-cell volume. The temperature evolution of the superstructure reflections follows a sigmoidal phase-fraction model that accounts for intermediate Na configurations and a region of phase coexistence, while calorimetry shows the largest configurational enthalpy release near 350 K.

What carries the argument

The redistribution of Na ions between the Na(1) and Na(2) sublattices inside a rigid [FeCr(PO4)3] polyanionic framework

Load-bearing premise

The observed symmetry change and intensity evolution are caused solely by Na-ion redistribution and not by undetected impurities, beam-induced effects, or incomplete modeling of the intermediate configurations.

What would settle it

High-resolution synchrotron or neutron diffraction data collected across the transition temperatures that show measurable shifts in the positions or thermal parameters of the Fe, Cr, P, or O atoms in the polyanionic framework would falsify the claim that the framework remains essentially unchanged.

Figures

Figures reproduced from arXiv: 2604.12828 by Archna Sagdeo, Madhav Sharma, Rajendra S. Dhaka.

Figure 1
Figure 1. Figure 1: FIG. 1. (a) The Rietveld-refined synchrotron XRD pattern, [PITH_FULL_IMAGE:figures/full_fig_p003_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: FIG. 2. (a) The differential scanning calorimetry (DSC) pro [PITH_FULL_IMAGE:figures/full_fig_p004_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: FIG. 3. The Rietveld refined synchrotron XRD patterns collected at (a) 303 K and fitted with the monoclinic [PITH_FULL_IMAGE:figures/full_fig_p005_3.png] view at source ↗
Figure 4
Figure 4. Figure 4: FIG. 4. (a) The three-dimensional map of intensity showing the evolution of diffraction peaks with temperature collected during [PITH_FULL_IMAGE:figures/full_fig_p007_4.png] view at source ↗
Figure 5
Figure 5. Figure 5: FIG. 5. (a) The temperature evolution of the integrated in [PITH_FULL_IMAGE:figures/full_fig_p009_5.png] view at source ↗
read the original abstract

We report the temperature-dependent synchrotron based X-ray diffraction analysis of NASICON type Na$_3$FeCr(PO$_4$)$_3$ sample, which undergoes a symmetry-lowering structural transition from a monoclinic ($C2/c$) phase with long-range Na-vacancy order to a rhombohedral ($R\bar{3}c$) phase with statistical disordered Na ions. The [FeCr(PO$_4$)$_3$] polyanionic framework remains essentially unchanged, confirming that the transition is governed by redistribution of the Na sublattice rather than by reconstruction of the host framework. The structural evolution is accompanied by a discontinuous increase in the $c$-axis and the unit-cell volume, reflecting the progressive depopulation of the Na(1) sites and transfer of Na ions toward the Na(2) sublattice. The temperature dependence of superstructure intensity found to deviate from mean-field critical behavior, instead, the experimental evolution is accurately captured by a sigmoidal phase-fraction model. The calorimetric measurements show that the enthalpy change for the first transition around 350~K is significantly larger than that of the anomaly around 445 K, indicating the dominant configurational rearrangement of Na ions occurs within the lower-temperature interval. Overall, the diffraction and calorimetric results demonstrate that Na ordering proceeds through an order-disorder transition involving intermediate Na configurations and a finite coexisting regime. The quantitative correlation between Na-vacancy ordering, lattice strain, and symmetry lowering reveals the central role of configurational interactions within the Na conduction channels in governing the phase stability of NASICON-type materials.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

1 major / 2 minor

Summary. The manuscript reports temperature-dependent synchrotron XRD and calorimetry on NASICON-type Na₃FeCr(PO₄)₃, documenting a first-order symmetry-lowering transition from monoclinic C2/c (long-range Na-vacancy order) to rhombohedral R-3c (disordered Na ions) near 350 K. The central claim is that the [FeCr(PO₄)₃] polyanionic framework remains essentially unchanged while Na ions redistribute from Na(1) to Na(2) sites, producing a discontinuous c-axis and volume increase; superstructure intensity evolution is captured by a sigmoidal phase-fraction model rather than mean-field behavior, and calorimetry shows larger enthalpy change at the lower-temperature transition, indicating dominant configurational Na rearrangement.

Significance. If the framework-invariance claim is quantitatively confirmed, the work strengthens the understanding that Na-sublattice configurational interactions, rather than host-framework reconstruction, control phase stability and ion-transport properties in NASICON materials. The combination of high-resolution diffraction, clear space-group assignments, observed volume jumps, and non-mean-field intensity modeling provides useful experimental constraints on intermediate Na configurations; this has direct relevance for designing Na-ion conductors.

major comments (1)
  1. [Rietveld refinements and structural discussion] Rietveld refinements and structural discussion (results section): The central assertion that the [FeCr(PO₄)₃] polyanionic framework remains essentially unchanged is load-bearing for the interpretation yet unsupported by quantitative metrics. No tabulated or plotted values are given for changes in P–O, Fe–O or Cr–O bond lengths, O–P–O angles, or polyhedral volumes between the C2/c and R-3c refinements, nor any statistical test (e.g., Δd < 3σ) confirming invariance within error. Without these, small symmetry-breaking distortions cannot be excluded as co-drivers of the observed intensity evolution and symmetry change.
minor comments (2)
  1. [Abstract] Abstract: the sentence 'The temperature dependence of superstructure intensity found to deviate from mean-field critical behavior' is grammatically incomplete and should read 'is found to deviate'.
  2. [Results] The manuscript would benefit from explicit statement of the temperature range and number of data points used in the sigmoidal phase-fraction fit, and from a direct comparison of the fit residuals to a mean-field model.

Simulated Author's Rebuttal

1 responses · 0 unresolved

We thank the referee for their thorough review and insightful comments on our manuscript. We address the major comment below and will incorporate the requested quantitative analysis in a revised version to strengthen the structural interpretation.

read point-by-point responses
  1. Referee: [Rietveld refinements and structural discussion] Rietveld refinements and structural discussion (results section): The central assertion that the [FeCr(PO₄)₃] polyanionic framework remains essentially unchanged is load-bearing for the interpretation yet unsupported by quantitative metrics. No tabulated or plotted values are given for changes in P–O, Fe–O or Cr–O bond lengths, O–P–O angles, or polyhedral volumes between the C2/c and R-3c refinements, nor any statistical test (e.g., Δd < 3σ) confirming invariance within error. Without these, small symmetry-breaking distortions cannot be excluded as co-drivers of the observed intensity evolution and symmetry change.

    Authors: We agree that the manuscript would benefit from explicit quantitative metrics to support the framework-invariance claim. In the revised manuscript, we will add a dedicated table (and associated text in the results section) comparing P–O, Fe–O, and Cr–O bond lengths, O–P–O angles, and polyhedral volumes between the C2/c and R-3c refinements at temperatures immediately below and above the transition. We will also report the differences with their estimated standard deviations and include a note confirming that all changes lie within 3σ, thereby demonstrating that the polyanionic framework remains essentially unchanged within experimental error. This addition will directly address the possibility of small symmetry-breaking distortions. revision: yes

Circularity Check

0 steps flagged

No circularity in experimental structural analysis

full rationale

This is a purely observational experimental paper reporting synchrotron XRD and calorimetric data on a NASICON material's order-disorder transition. The central claim that the [FeCr(PO4)3] framework remains unchanged while Na redistributes follows directly from Rietveld refinements of the diffraction patterns and from the measured enthalpy changes; no mathematical derivation, fitted parameter renamed as prediction, or self-citation chain is invoked to reach the conclusion. The sigmoidal phase-fraction model is presented only as a descriptive fit to the observed superstructure intensity evolution, not as an independent prediction. All load-bearing steps rest on external experimental observables rather than on any reduction to the paper's own inputs by construction.

Axiom & Free-Parameter Ledger

0 free parameters · 1 axioms · 0 invented entities

Experimental study with no free parameters, no invented entities, and only standard crystallographic assumptions.

axioms (1)
  • standard math Space-group assignments from diffraction patterns correctly identify monoclinic C2/c and rhombohedral R-3c phases.
    Invoked when indexing superstructure reflections and tracking symmetry lowering.

pith-pipeline@v0.9.0 · 5611 in / 1190 out tokens · 36787 ms · 2026-05-10T14:38:40.090202+00:00 · methodology

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Reference graph

Works this paper leans on

43 extracted references · 43 canonical work pages

  1. [1]

    T. Jin, H. Li, K. Zhu, P.-F. Wang, P. Liu, and L. Jiao, Polyanion-type cathode materials for sodium-ion batter- ies, Chem. Soc. Rev.49, 2342 (2020)

  2. [2]

    Sharma, R

    M. Sharma, R. Gulati, and R. S. Dhaka, Synergistic role of transition metals and polyanionic frameworks in phosphate-based cathode materials for sodium-ion bat- teries, Coord. Chem. Rev.543, 216912 (2025)

  3. [3]

    C. Liu, Z. G. Neale, and G. Cao, Understanding electro- chemical potentials of cathode materials in rechargeable batteries, Materials Today19, 109 (2016)

  4. [4]

    Park, J.-N

    S. Park, J.-N. Chotard, D. Carlier, I. Moog, M. Courty, M. Duttine, F. Fauth, A. Iadecola, L. Croguennec, and C. Masquelier, Crystal structures and local environments of NASICON-type Na 3FeV(PO4)3 and Na 4FeV(PO4)3 positive electrode materials for Na-ion batteries, Chem. Mater.33, 5355 (2021)

  5. [5]

    L. Yang, X. Yin, J. Wang, Y. Sun, Y. Li, Z. Zhang, Z. Liu, S.-M. Huang, P. Adelhelm, and D. Zhou, Sub- stitution and electrochemistry in layered oxide cathode materials for sodium-ion batteries, Nat. Rev. Chem.10, 196 (2026)

  6. [6]

    G. Yan, S. Mariyappan, G. Rousse, Q. Jacquet, M. Deschamps, R. David, B. Mirvaux, J. W. Freeland, and J.-M. Tarascon, Higher energy and safer sodium ion batteries via an electrochemically made disordered Na3V2(PO4)2F3 material, Nat. Commun.10, 585 (2019)

  7. [7]

    Nishimura, R

    S. Nishimura, R. Natsui, and A. Yamada, Superstructure in the metastable intermediate-phase Li 2/3FePO4 accel- erating the lithium battery cathode reaction, Angew. Chem. Int. Ed.54, 8939 (2015)

  8. [8]

    Boucher, J

    F. Boucher, J. Gaubicher, M. Cuisinier, D. Guy- omard, and P. Moreau, Elucidation of the Na 2/3FePO4 and Li 2/3FePO4 intermediate superstructure revealing a pseudouniform ordering in 2D, J. Am. Chem. Soc.136, 9144 (2014)

  9. [9]

    G. J. Redhammer, G. Tippelt, Q. Stahl, A. Benisek, and D. Rettenwander, Study on the structural phase transi- tions in NaSICON-type compounds using Ag 3Sc2(PO4)3 as a model system, Acta Crystallogr. B Struct. Sci. Cryst. Eng. Mater.77, 10 (2021)

  10. [10]

    Y. Wang, J. Jin, X. Zhao, Q. Shen, X. Qu, L. Jiao, and Y. Liu, Unexpected elevated working voltage by Na+/vacancy ordering and stabilized sodium-ion storage by transition-metal honeycomb ordering, Angew. Chem. Int. Ed.63, e202409152 (2024)

  11. [11]

    P. -F. Wang, H.-R. Yao, X.-Y. Liu, Y.-X. Yin, J.- N. Zhang, Y. Wen, X. Yu, L. Gu, and Y.-G. Guo, Na+/vacancy disordering promises high-rate Na-ion bat- teries, Sci. Adv.4, eaar6018 (2018)

  12. [12]

    B. C. Melot, D. O. Scanlon, M. Reynaud, G. Rousse, J.-N. Chotard, M. Henry, and J. -M. Tarascon, Chemi- cal and structural indicators for large redox potentials in Fe-based positive electrode materials, ACS Appl. Mater. Interfaces6, 10832 (2014)

  13. [13]

    Y. Shi, P. Jiang, S. Wang, W. Chen, B. Wei, X. Lu, G. Qian, W. H. Kan, H. Chen, W. Yin, Y. Sun and X. Lu, Slight compositional variation-induced structural disorder-to-order transition enables fast Na + storage in layered transition metal oxides, Nat. Commun.13, 7888 (2022)

  14. [14]

    Y. He, E. Scivally, A. Shaji, B. Ouyang, and Y. Zeng, Unraveling the fast ionic conduction in NASICON-type materials, Adv. Energy Mater.15, 2403877 (2025). 12

  15. [15]

    S. K. Sapra, J. Pati, P. K. Dwivedi, S. Basu, J. Chang, and R. S. Dhaka, A comprehensive review on recent ad- vances of polyanionic cathode materials in Na-ion batter- ies for cost effective energy storage applications, WIREs Energy & Environment10, e400 (2021)

  16. [16]

    Meena and R

    R. Meena and R. S. Dhaka, Structural and elec- trical transport properties of NASICON type Na3Zr2−xTixSi2PO12 ( x = 0.1-0.4) solid electrolyte materials, Small21, 2501197 (2025)

  17. [17]

    Sharma and R

    M. Sharma and R. S. Dhaka, Electrochemical per- formance and diffusion kinetics of a NASICON type Na3.3Mn1.2Ti0.75Mo0.05(PO4)3/C cathode for low-cost sodium-ion batteries, Small21, 2505200 (2025)

  18. [18]

    H. Y.-P. Hong, Crystal structures and crystal chemistry in the system Na 1+xZr2SixP3−xO12, Mater. Res. Bull. 11, 173 (1976)

  19. [19]

    Kabbour, D

    H. Kabbour, D. Coillot, M. Colmont, C. Masquelier, and O. Mentr´ e,α-Na 3M2(PO4)3 (M = Ti, Fe): abso- lute cationic ordering in NASICON-type phases, J. Am. Chem. Soc.133, 11900 (2011)

  20. [20]

    d ′Yvoire, M

    F. d ′Yvoire, M. Pintard-Scr´ epel, E. Bretey, and M. De La Roch` ere, Phase transitions and ionic conduction in 3D skeleton phosphates A 3M2(PO4)3 : A = Li, Na, Ag, K; M = Cr, Fe, Solid State Ionics9-10, 851 (1983)

  21. [21]

    Chotard, G

    J.-N. Chotard, G. Rousse, R. David, O. Mentr´ e, M. Courty, and C. Masquelier, Discovery of a sodium- ordered form of Na 3V2(PO4)3 below ambient tempera- ture, Chem. Mater.27, 5982 (2015)

  22. [22]

    S. Park, J. -N. Chotard, D. Carlier, I. Moog, M. Duttine, F. Fauth, A. Iadecola, L. Croguennec, and C. Masquelier, An asymmetric sodium extraction/insertion mechanism for the Fe/V-mixed NASICON Na 4FeV(PO4)3, Chem. Mater.34, 4142 (2022)

  23. [23]

    J. Wang, T. He, X. Yang, Z. Cai, Y. Wang, V. Lacivita, H. Kim, B. Ouyang, and G. Ceder, Design principles for NASICON super-ionic conductors, Nat. Commun.14, 5210 (2023)

  24. [24]

    Masquelier, C

    C. Masquelier, C. Wurm, J. Rodr´ ıguez-Carvajal, J. Gaubicher, and L. Nazar, A powder neutron diffrac- tion investigation of the two rhombohedral NASICON analogues:γ-Na 3Fe2(PO4)3 and Li 3Fe2(PO4)3, Chem. Mater.12, 525 (2000)

  25. [25]

    M. Kr. Singh, A. K. Bera, A. Kumar, S. M. Yusuf, and R. S. Dhaka, Antiferromagnetic ordering and glassy nature in the sodium superionic conductor NaFe 2PO4(SO4)2, Phys. Rev. B109, 174401 (2024)

  26. [26]

    See Supplemental Material for further information about Bond valence sum (BVS), Local distortion (∆), FESEM image, mass sum spectra, EDX images, Raman modes as- signment, intralayer distribution of Na ions, and Rietveld refined XRD patterns at each temperature

  27. [27]

    H. Bih, L. Bih, B. Manoun, M. Azdouz, S. Benmokhtar, and P. Lazor, Raman spectroscopic study of the phase transitions sequence in Li3Fe2(PO4)3 and Na3Fe2(PO4)3 at high temperature, J. Mol. Struct.936, 147 (2009)

  28. [28]

    M. Barj, G. Lucazeau, and C. Delmas, Raman and in- frared spectra of some chromium Nasicon-type materi- als: Short-range disorder characterization, J. Solid State Chem.100, 141 (1992)

  29. [29]

    Sharma, P

    M. Sharma, P. Sindhu, and R. S. Dhaka, Case study of an exploratory high voltage NASICON-based Na4NiCr(PO4)3 cathode material for sodium-ion batter- ies, arXiv:2601.07012

  30. [30]

    M. C. Biesinger, C. Brown, J. R. Mycroft, R. D. David- son, and N. S. McIntyre, X-ray photoelectron spec- troscopy studies of chromium compounds, Surf. Interface Anal.36, 1550 (2004)

  31. [31]

    P. H. Citrin, High-resolution x-ray photoemission from sodium metal and its hydroxide, Phys. Rev. B8, 5545 (1973)

  32. [32]

    Kumar, R

    A. Kumar, R. Shukla, A. Pandey, S. Dalal, M. Miryala, K. Ueno, M. Murakami, and R. S. Dhaka, Struc- tural, transport, optical, and electronic properties of Sr2CoNbO6 thin films, J. Appl. Phys.128, 025303 (2020)

  33. [33]

    Z. Wang, S. Park, Z. Deng, D. Carlier, J.-N. Chotard, L. Croguennec, G. S. Gautam, A. K. Cheetham, C. Masque- lier, and P. Canepa, Phase stability and sodium-vacancy orderings in a NaSICON electrode, J. Mater. Chem. A 10, 209 (2022)

  34. [34]

    Kumar, A

    A. Kumar, A. Jain, S. M. Yusuf, and R. S. Dhaka, Ob- servation of anisotropic thermal expansion and the Jahn- Teller effect in double perovskites Sr 2−xLaxCoNbO6 Us- ing Neutron Diffraction, J. Phys. Chem. Lett.13, 3023 (2022)

  35. [35]

    W. L. Bragg and E. J. Williams, The effect of thermal agitation on atomic arrangement in alloys, Proceedings of the Royal Society of London. Series A, Containing Pa- pers of a Mathematical and Physical Character145, 699 (1934)

  36. [36]

    K. R. Subbaswamy and D. L. Mills, Simple model of a structural phase transition of the order-disorder type, Phys. Rev. B18, 1446 (1978)

  37. [37]

    L. S. I. Veiga, J. R. L. Mardegan, M. V. Zimmermann, D. T. Maimone, F. B. Carneiro, M. B. Fontes, J. Strempfer, E. Granado, P. G. Pagliuso, and E. M. Bittar, Possi- ble quantum fluctuations in the vicinity of the quantum critical point of (Sr, Ca)3Ir4Sn13 revealed by high-energy x-ray diffraction, Phys. Rev. B101, 104511 (2020)

  38. [38]

    S. K. Mishra, R. Mittal, V. Yu. Pomjakushin, and S. L. Chaplot, Phase stability and structural temperature dependence in sodium niobate: A high-resolution pow- der neutron diffraction study, Phys. Rev. B83, 134105 (2011)

  39. [39]

    A. G. Khachaturyan, Theory of structural transforma- tions in solids. (Dover Publications, Newburyport, 2013)

  40. [40]

    Chen, Chemical potential and Gibbs free energy, MRS Bulletin44, 520 (2019)

    L.- Q. Chen, Chemical potential and Gibbs free energy, MRS Bulletin44, 520 (2019)

  41. [41]

    S. M. Sharma and Y. M. Gupta, Inherent issues regarding the use of in situ x-ray diffraction measurements to de- termine temperature in shock-compressed metals, Phys. Rev. B104, 064113 (2021)

  42. [42]

    Dolabella, A

    S. Dolabella, A. Borz` ı, A. Dommann, and A. Neels, Lat- tice strain and defects analysis in nanostructured semi- conductor materials and devices by high-resolution x- ray diffraction: theoretical and practical aspects, Small Methods6, 2100932 (2022)

  43. [43]

    H. Abe, H. Saitoh, T. Ueno, H. Nakao, Y. Matsuo, K. Ohshima, and H. Matsumoto, Diffuse scattering from an Al72Ni20Co8 decagonal quasicrystal on an order disor- der transformation, J. Phys.: Condens. Matter15, 1665 (2003)